Answer and Solution:
As per the question:
Mass of each hobo is [tex]m_{h}[/tex]
Velocity of the either hobo is 'u'
Mass of the flatcar is [tex]m_{fc}[/tex]
Now,
(a) Suppose [tex]v_{r}[/tex] be the recoil velocity, then
Relative speed of either hobo w.r.t ground just after their jump is [tex]u - v_{r}[/tex]
Now, by the principle of conservation of momentum:
[tex]2m_{h}(u - v_{r}) = m_{fc}v_{r}[/tex]
[tex]v_{r} = \frac{2m_{h}}{m_{fc} + 2m_{h}}\times u[/tex] (1)
(b) Suppose the recoil velocity of the flatcar be [tex]v_{rc}[/tex] after the jump of the first hobo and [tex]v_{rc}[/tex] after the jump of the second hobo.
Now, applying the of conservation of momentum, after the jump of the first hobo is the same as done in part (a), but when only one hobo jumps, the mass of the second hobo remains:
[tex]m_{h(u - v_{rc})} = (m_{h} + m_{fc}}v_{rc})[/tex]
[tex]v_{rc} = \frac{m_{h}}{m_{fc} + 2m_{h}}\times u[/tex] (2)
Now, by conservation of momentum for the second jump:
[tex]m_{h}(u - v'_{rc}) - m_{fc}v'_{rc} = - (m_{fc} + m_{h})v_{rc}[/tex]
[tex]v'_{rc} = \frac{m_{h}u + (m_{h} + m_{fc})}{m_{h} + m_{fc}}\times v_{rc}[/tex] (3)
Now, from eqn (1), (2) and (3):
It is clear that [tex]v'_{rc}[/tex] > v_{rc}[tex][/tex]